无人机在未知环境避障中实时定位信号源并自适应导航
RF-Source Seeking with Obstacle Avoidance using Real-time Modified Artificial Potential Fields in Unknown Environments
- 基于采样调整势场参数,实现动态环境下的实时避障
- 仅用方向角估计,平均角度误差仅1.48度,成功率提升46%
- 适合搜救、巡检等信号源位置未知的复杂场景
在灾难救援和基础设施监测中,无人机在未知环境中避障导航至关重要。现有人工势场(APF)算法难以适应不同障碍物布局。在搜索救援等场景中,目标位置往往未知,可采用无线电(RF)信号源定位。本文提出一种实时轨迹规划方法:通过采样实现势场参数的实时自适应调整,仅依赖目标方向角而非精确位置,根据新障碍配置动态更新势场。主要贡献包括:(i) 基于天线布局计算的RF源定位算法,提供方向角估计;(ii) 可适配变化环境的改进型人工势场算法。在Gazebo仿真中使用ROS2通信,结果表明:该算法平均角度误差仅为1.48度;结合此估计,导航成功率提高46%,路径长度减少1.2%。
原文摘要 · Abstract (English)
Navigation of UAVs in unknown environments with obstacles is essential for applications in disaster response and infrastructure monitoring. However, existing obstacle avoidance algorithms, such as Artificial Potential Field (APF) are unable to generalize across environments with different obstacle configurations. Furthermore, the precise location of the final target may not be available in applications such as search and rescue, in which case approaches such as RF source seeking can be used to align towards the target location. This paper proposes a real-time trajectory planning method, which involves real-time adaptation of APF through a sampling-based approach. The proposed approach utilizes only the bearing angle of the target without its precise location, and adjusts the potential field parameters according to the environment with new obstacle configurations in real time. The main contributions of the article are i) an RF source seeking algorithm to provide a bearing angle estimate using RF signal calculations based on antenna placement, and ii) a modified APF for adaptable collision avoidance in changing environments, which are evaluated separately in the simulation software Gazebo, using ROS2 for communication. Simulation results show that the RF source-seeking algorithm achieves high accuracy, with an average angular error of just 1.48 degrees, and with this estimate, the proposed navigation algorithm improves the success rate of reaching the target by 46% and reduces the trajectory length by 1.2% compared to standard potential fields.
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